One may note that in the absence of a dilaton field where we have
\(V(\Phi )=2\Lambda =-6/l^2\) , the above counterterm has the same form
as in the case of asymptotically AdS solutions with zero-curvature
boundary. Having the total finite action \(I =I_{G}+I_{\mathrm {ct}}\)  at hand, one can use the quasilocal
definition to construct a divergence free stress-energy tensor
[1]}. Thus the finite stress-energy tensor in
four-dimensional Einstein-dilaton gravity with three
Liouville-type dilaton potentials (REF ) can be written as
\(T^{ab}=\frac{1}{8\pi }\left[ \Theta ^{ab}-\Theta \gamma ^{ab}+\left(-\frac{1}{l}+\frac{\sqrt{-6V(\Phi )}}{2} \right)\gamma ^{ab}\right]. \) 
